WO2014012945A1 - Procédé et dispositif de restitution d'une représentation de champs sonores audio pour une lecture audio - Google Patents

Procédé et dispositif de restitution d'une représentation de champs sonores audio pour une lecture audio Download PDF

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Publication number
WO2014012945A1
WO2014012945A1 PCT/EP2013/065034 EP2013065034W WO2014012945A1 WO 2014012945 A1 WO2014012945 A1 WO 2014012945A1 EP 2013065034 W EP2013065034 W EP 2013065034W WO 2014012945 A1 WO2014012945 A1 WO 2014012945A1
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WIPO (PCT)
Prior art keywords
matrix
decode
decode matrix
rendering
hoa
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Application number
PCT/EP2013/065034
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English (en)
Inventor
Johannes Boehm
Florian Keiler
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Thomson Licensing
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Filing date
Publication date
Priority to AU2013292057A priority Critical patent/AU2013292057B2/en
Priority to CN201380037816.5A priority patent/CN104584588B/zh
Application filed by Thomson Licensing filed Critical Thomson Licensing
Priority to JP2015522078A priority patent/JP6230602B2/ja
Priority to EP19203226.6A priority patent/EP3629605B1/fr
Priority to KR1020207004422A priority patent/KR102201034B1/ko
Priority to BR122020017389-0A priority patent/BR122020017389B1/pt
Priority to KR1020227044216A priority patent/KR102597573B1/ko
Priority to KR1020217000214A priority patent/KR102479737B1/ko
Priority to BR122020017399-8A priority patent/BR122020017399B1/pt
Priority to EP21214639.3A priority patent/EP4013072B1/fr
Priority to BR112015001128-4A priority patent/BR112015001128B1/pt
Priority to KR1020157000821A priority patent/KR102079680B1/ko
Priority to US14/415,561 priority patent/US9712938B2/en
Priority to KR1020237037407A priority patent/KR20230154111A/ko
Priority to EP23202235.0A priority patent/EP4284026A3/fr
Priority to EP13737262.9A priority patent/EP2873253B1/fr
Publication of WO2014012945A1 publication Critical patent/WO2014012945A1/fr
Priority to HK15111315.8A priority patent/HK1210562A1/xx
Priority to AU2017203820A priority patent/AU2017203820B2/en
Priority to US15/619,935 priority patent/US9961470B2/en
Priority to US15/920,849 priority patent/US10075799B2/en
Priority to US16/114,937 priority patent/US10306393B2/en
Priority to AU2019201900A priority patent/AU2019201900B2/en
Priority to US16/417,515 priority patent/US10595145B2/en
Priority to US16/789,077 priority patent/US10939220B2/en
Priority to US17/189,067 priority patent/US11451920B2/en
Priority to AU2021203484A priority patent/AU2021203484B2/en
Priority to US17/943,965 priority patent/US11743669B2/en
Priority to AU2023203838A priority patent/AU2023203838A1/en
Priority to US18/359,198 priority patent/US20240040327A1/en

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Classifications

    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04S—STEREOPHONIC SYSTEMS 
    • H04S7/00—Indicating arrangements; Control arrangements, e.g. balance control
    • H04S7/30—Control circuits for electronic adaptation of the sound field
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04S—STEREOPHONIC SYSTEMS 
    • H04S3/00—Systems employing more than two channels, e.g. quadraphonic
    • H04S3/008—Systems employing more than two channels, e.g. quadraphonic in which the audio signals are in digital form, i.e. employing more than two discrete digital channels
    • H—ELECTRICITY
    • H04—ELECTRIC COMMUNICATION TECHNIQUE
    • H04S—STEREOPHONIC SYSTEMS 
    • H04S2420/00—Techniques used stereophonic systems covered by H04S but not provided for in its groups
    • H04S2420/11—Application of ambisonics in stereophonic audio systems

Definitions

  • This invention relates to a method and a device for rendering an audio soundfield representation, and in particular an Ambisonics formatted audio representation, for audio playback.
  • Ambisonics carry a representation of a desired sound field.
  • the Ambisonics format is based on spherical harmonic decomposition of the soundfield. While the basic Ambisonics format or B-format uses spherical harmonics of order zero and one, the so-called Higher Order Ambisonics (HOA) uses also further spherical harmonics of at least 2 nd order.
  • a decoding or rendering process is required to obtain the individual loudspeaker signals from such Ambisonics formatted signals.
  • the spatial arrangement of loudspeakers is referred to as loudspeaker setup herein.
  • known rendering approaches are suitable only for regular loudspeaker setups, arbitrary loudspeaker setups are much more common. If such rendering approaches are applied to arbitrary loudspeaker setups, sound directivity suffers.
  • the present invention describes a method for rendering/decoding an audio sound field representation for both regular and non-regular spatial loudspeaker distributions, where the rendering/decoding provides highly improved localization properties and is energy preserving.
  • the invention provides a new way to obtain the decode matrix for sound field data, e.g. in HOA format. Since the HOA format describes a sound field, which is not directly related to loudspeaker positions, and since loudspeaker signals to be obtained are necessarily in a channel-based audio format, the decoding of HOA signals is always tightly related to rendering the audio signal. Therefore the present invention relates to both decoding and rendering sound field related audio formats.
  • One advantage of the present invention is that energy preserving decoding with very good directional properties is achieved.
  • energy preserving means that the energy within the HOA directive signal is preserved after decoding, so that e.g. a constant amplitude directional spatial sweep will be perceived with constant loudness.
  • good directional properties refers to the speaker directivity characterized by a directive main lobe and small side lobes, wherein the directivity is increased compared with conventional rendering/decoding.
  • the invention discloses rendering sound field signals, such as Higher-Order Ambisonics (HOA), for arbitrary loudspeaker setups, where the rendering results in highly improved localization properties and is energy preserving. This is obtained by a new type of decode matrix for sound field data, and a new way to obtain the decode matrix.
  • HOA Higher-Order Ambisonics
  • the decode matrix for the rendering to a given arrangement of target loudspeakers is obtained by steps of obtaining a number of target speakers and their positions, positions of a spherical modeling grid and a HOA order, generating a mix matrix from the positions of the modeling grid and the positions of the speakers, generating a mode matrix from the positions of the spherical modeling grid and the HOA order, calculating a first decode matrix from the mix matrix and the mode matrix, and smoothing and scaling the first decode matrix with smoothing and scaling coefficients to obtain an energy preserving decode matrix.
  • the invention relates to a method for decoding and/or rendering an audio sound field representation for audio playback as claimed in claim 1 .
  • the invention relates to a device for decoding and/or rendering an audio sound field representation for audio playback as claimed in claim 9.
  • the invention relates to a computer readable medium having stored on it executable instructions to cause a computer to perform a method for decoding and/or rendering an audio sound field representation for audio playback as claimed in claim 15.
  • the invention uses the following approach.
  • panning functions are derived that are dependent on a loudspeaker setup that is used for playback.
  • a decode matrix e.g. Ambisonics decode matrix
  • the decode matrix is generated and processed to be energy preserving.
  • the decode matrix is filtered in order to smooth the loudspeaker panning main lobe and suppress side lobes. The filtered decode matrix is used to render the audio signal for the given loudspeaker setup. Side lobes are a side effect of rendering and provide audio signals in unwanted directions.
  • a method for rendering/decoding an audio sound field representation for audio playback comprises steps of buffering received HOA time samples b(t), wherein blocks of M samples and a time index ⁇ are formed, filtering the coefficients ⁇ ( ⁇ ) to obtain frequency filtered coefficients ⁇ ( ⁇ ) , rendering the frequency filtered coefficients ⁇ ( ⁇ ) to a spatial domain using a decode matrix D, wherein a spatial signal ⁇ ( ⁇ ) is obtained.
  • further steps comprise delaying the time samples w(t) individually for each of the L channels in delay lines, wherein L digital signals are obtained, and Digital-to-Analog (D/A) converting and amplifying the L digital signals, wherein L analog loudspeaker signals are obtained.
  • the decode matrix D for the rendering step i.e.
  • the decode matrix for rendering to a given arrangement of target speakers, is obtained by steps of obtaining a number of target speakers and positions of the speakers, determining positions of a spherical modeling grid and a HOA order, generating a mix matrix from the positions of a spherical modeling grid and the positions of the speakers, generating a mode matrix from the spherical modeling grid and the HOA order, calculating a first decode matrix from the mix matrix G and the mode matrix ⁇ , and smoothing and scaling the first decode matrix with smoothing and scaling coefficients, wherein the decode matrix is obtained.
  • a computer readable medium has stored on it executable instructions that when executed on a computer cause the computer to perform a method for decoding an audio sound field representation for audio playback as disclosed above.
  • Fig.1 a flow-chart of a method according to one embodiment of the invention
  • Fig.2 a flow-chart of a method for building the mix matrix G
  • Fig.3 a block diagram of a renderer
  • Fig.4 a flow-chart of schematic steps of a decode matrix generation process
  • Fig.5 a block diagram of a decode matrix generation unit
  • Fig.6 an exemplary 16-speaker setup, where speakers are shown as connected nodes;
  • Fig.7 the exemplary 16-speaker setup in natural view, where nodes are shown as
  • Fig.8 an energy diagram showing the E/E ratio being constant for perfect energy
  • Fig.12 an energy diagram showing the E/E ratio having fluctuations smaller than 1 dB as obtained by a method or apparatus according to the invention, where spatial pans with constant amplitude are perceived with equal loudness;
  • Fig.13 a sound pressure diagram for a decode matrix designed with the method
  • the center speaker has a panning beam with small side lobes.
  • the invention relates to rendering (i.e. decoding) sound field formatted audio signals such as Higher Order Ambisonics (HOA) audio signals to loudspeakers, where the loudspeakers are at symmetric or asymmetric, regular or non-regular positions.
  • the audio signals may be suitable for feeding more loudspeakers than available, e.g. the number of HOA coefficients may be larger than the number of loudspeakers.
  • the invention provides energy preserving decode matrices for decoders with very good directional properties, i.e. speaker directivity lobes generally comprise a stronger directive main lobe and smaller side lobes than speaker directivity lobes obtained with
  • Energy preserving means that the energy within the HOA directive signal is preserved after decoding, so that e.g. a constant amplitude directional spatial sweep will be perceived with constant loudness.
  • Fig.1 shows a flow-chart of a method according to one embodiment of the invention.
  • the method for rendering (i.e. decoding) a HOA audio sound field representation for audio playback uses a decode matrix that is generated as follows: first, a number L of target loudspeakers, the positions D L of the loudspeakers, a spherical modeling grid D s and an order N (e.g. HOA order) are determined 1 1 . From the positions D L of the speakers and the spherical modeling grid D s , a mix matrix G is generated 12, and from the spherical modeling grid D s and the HOA order N, a mode matrix ⁇ is generated 13.
  • a decode matrix that is generated as follows: first, a number L of target loudspeakers, the positions D L of the loudspeakers, a spherical modeling grid D s and an order N (e.g. HOA order) are determined 1 1 . From the positions D L of the speakers and the
  • a first decode matrix D is calculated 14 from the mix matrix G and the mode matrix ⁇ .
  • the first decode matrix D is smoothed 15 with smoothing coefficients A , wherein a smoothed decode matrix D is obtained, and the smoothed decode matrix D is scaled 16 with a scaling factor obtained from the smoothed decode matrix D, wherein the decode matrix D is obtained.
  • the smoothing 15 and scaling 16 is performed in a single step.
  • a plurality of decode matrices corresponding to a plurality of different loudspeaker arrangements are generated and stored for later usage.
  • the different loudspeaker arrangements can differ by at least one of the number of loudspeakers, a position of one or more loudspeakers and an order N of an input audio signal. Then, upon initializing the rendering system, a matching decode matrix is determined, retrieved from the storage according to current needs, and used for decoding.
  • the U,V are derived from Unitary matrices, and S is a diagonal matrix with singular value elements of said compact singular value decomposition of the product of the mode matrix ⁇ with the Hermitian transposed mix matrix G H .
  • Decode matrices obtained according to this embodiment are often numerically more stable than decode matrices obtained with an alternative embodiment described below.
  • the Hermitian transposed of a matrix is the conjugate complex transposed of the matrix.
  • the threshold thr depends on the actual values of the singular value decomposition matrix and may be, exemplarily, in the order of 0,06 * Si (the maximum element of S).
  • the S and threshold thr are as described above for the previous embodiment.
  • the threshold thr is usually derived from the largest singular value.
  • A Cf [K N+1 , K N+2 , ⁇ : N+ 2, ⁇ : N + 2, ⁇ : N+3 , K N+3 , ... , K 2N Y with a scaling factor c f .
  • the used elements of the Kaiser window begin with the (N+1 ) st element, which is used only once, and continue with subsequent elements which are used repeatedly: the (N+2) nd element is used three times, etc.
  • the scaling factor is obtained from the smoothed decoding matrix. In particular, in one embodiment it is obtained according to
  • a major focus of the invention is the initialization phase of the renderer, where a decode matrix D is generated as described above.
  • the main focus is a technology to derive the one or more decoding matrices, e.g. for a code book.
  • For generating a decode matrix it is known how many target loudspeakers are available, and where they are located (i.e. their positions).
  • Fig.2 shows a flow-chart of a method for building the mix matrix G, according to one embodiment of the invention.
  • the following section gives a brief introduction to Higher Order Ambisonics (HOA) and defines the signals to be processed, i.e. rendered for loudspeakers.
  • HOA Higher Order Ambisonics
  • HOA Higher Order Ambisonics
  • ⁇ ( ⁇ , ⁇ ) T t ⁇ p ⁇ t, x) ) (1 )
  • ⁇ denotes the angular frequency (and T t ⁇ ) corresponds to /_ ⁇ p(t, x) e ⁇ ⁇ )
  • SHs Spherical Harmonics
  • SHs are complex valued functions in general. However, by an appropriate linear combination of them, it is possible to obtain real valued functions and perform the expansion with respect to these functions.
  • a source field can be defined as:
  • a source field can consist of far-field/ near- field, discrete/continuous sources [1].
  • the source field coefficients BTM are related to the sound field coefficients ATM by, [1 ]: for the far field
  • the coefficients bTM comprise the Audio information of one time sample t for later reproduction by loudspeakers. They can be stored or transmitted and are thus subject of data rate compression.
  • metadata is sent along the coefficient data, allowing an
  • w D b (9) where w e I L X L represents a time sample of L speaker signals and decode matrix D e C LX ° 3D .
  • a decode matrix can be derived by
  • ⁇ ⁇ + ( 1 °)
  • ⁇ + is the pseudo inverse of the mode matrix ⁇ .
  • the mode-matrix ⁇ is defined as
  • Spherical convolution can be used for spatial smoothing. This is a spatial filtering process, or a windowing in the coefficient domain (convolution). Its purpose is to minimize the side lobes, so-called panning lobes.
  • a new coefficient bTM is given by the weighted product of the original H nal coefficient h° [5]:
  • weighting coefficients and a constant factor df are so called max r v , max r E and inphase coefficients [4].
  • a renderer architecture is described in terms of its initialization, start-up behavior and processing.
  • the renderer Every time the loudspeaker setup, i.e. the number of loudspeakers or position of any loudspeaker relative to the listening position changes, the renderer needs to perform an initialization process to determine a set of decoding matrices for any HOA-order N that supported HOA input signals have. Also the individual speaker delays d t for the delay lines and speaker gains g> x are determined from the distance between a speaker and a listening position. This process is described below.
  • the derived decoding matrices are stored within a code book. Every time the HOA audio input characteristics change, a renderer control unit determines currently valid characteristics and selects a matching decode matrix from the code book. Code book key can be the HOA order N or, equivalently, 0 3D (see eq.(6)).
  • Fig.3 shows a block diagram of processing blocks of the renderer. These are a first buffer 31 , a Frequency Domain Filtering unit 32, a rendering processing unit 33, a second buffer 34, a delay unit 35 for L channels, and a digital-to-analog converter and amplifier 36.
  • the HOA time samples with time-index t and 0 3D HOA coefficient channels b(i) are first stored in the first buffer 31 to form blocks of M samples with block index ⁇ .
  • the coefficients of ⁇ ( ⁇ ) are frequency filtered in the Frequency Domain Filtering unit 32 to obtain frequency filtered blocks ⁇ ( ⁇ ). This technology is known (see [3]) for
  • the frequency filtered block signals ⁇ ( ⁇ ) are rendered to the spatial domain in the rendering processing unit 33 by.
  • W(ji) D ⁇ ) (19) with 1 ⁇ ( ⁇ ) e I Lx representing a spatial signal in L channels with blocks of M time samples.
  • the signal is buffered in the second buffer 34 and serialized to form single time samples with time index t in L channels, referred to as w(t) in Fig.3.
  • This is a serial signal that is fed to L digital delay lines in the delay unit 35.
  • the delay lines compensate for different distances of listening position to individual speaker I with a delay of d t samples.
  • each delay line is a FIFO (first-in-first-out memory).
  • the delay compensated signals 355 are D/A converted and amplified in the digital-to-analog converter and amplifier 36, which provides signals 365 that can be fed to L loudspeakers.
  • the speaker gain compensation g> x can be considered before D/A conversion or by adapting the speaker channel amplification in analog domain.
  • the renderer initialization works as follows.
  • Various methods may apply, e.g. manual input of the speaker positions or automatic initialization using a test signal. Manual input of the speaker positions D L may be done using an adequate interface, like a connected mobile device or an device-integrated user-interface for selection of predefined position sets.
  • Automatic initialization may be done using a microphone array and dedicated speaker test signals with an evaluation unit to derive D L .
  • the L distances and r max are input to the delay line and gain compensation 35.
  • the number of delay samples for each speaker channel d t are determined by
  • Fig.4 shows, in one embodiment, processing blocks of a corresponding device for generating the decode matrix.
  • Inputs are speaker directions D L , a spherical modeling grid D s and the HOA-order N.
  • the speaker directions D L [ ⁇ 1( ... , n L ] can be expressed as spherical angles
  • the speaker directions D L and the spherical modeling grid D s are input to a Build Mix- Matrix block 41 , which generates a mix matrix G thereof.
  • the a spherical modeling grid D s and the HOA order N are input to a Build Mode-Matrix block 42, which generates a mode matrix ⁇ thereof.
  • the mix matrix G and the mode matrix ⁇ are input to a Build Decode Matrix block 43, which generates a decode matrix D thereof.
  • the decode matrix is input to a Smooth Decode Matrix block 44, which smoothes and scales the decode matrix. Further details are provided below.
  • Output of the Smooth Decode Matrix block 44 is the decode matrix D, which is stored in the code book with related key N (or alternatively 0 3D ).
  • a mix matrix G is created with G e I LxS . It is noted that the mix matrix G is referred to as W ' m [2].
  • An Z th row of the mix matrix G consists of mixing gains to mix S virtual sources from directions D s to speaker I.
  • Vector Base Amplitude Panning (VBAP) [1 1 ] is used to derive these mixing gains, as also in [2].
  • the algorithm to derive G is summarized in the following.
  • the compact singular value decomposition of the matrix product of the mode matrix and the transposed mixing matrix is calculated. This is an important aspect of the present invention, which can be performed in various manners.
  • the compact singular value decomposition S of the matrix product of the mode matrix ⁇ and the transposed mixing matrix G T is calculated according to:
  • the compact singular value decomposition S of the matrix product of the mode matrix ⁇ and the pseudo-inverse mixing matrix G + is calculated according to:
  • G + is the pseudo-inverse of mixing matrix G.
  • a suitable threshold value was found to be around 0.06. Small deviations e.g. within a range of ⁇ 0.01 or a range of ⁇ 1 0% are acceptable.
  • the decode matrix is smoothed. Instead of applying smoothing coefficients to the HOA coefficients before decoding, as known in prior art, it can be combined directly with the decode matrix. This saves one processing step, or processing block respectively.
  • A corresponds to max r E coefficients derived from the zeros of the
  • the elements are created by the Kaiser window formula where 7 0 ( ) denotes the zero-order Modified Bessel function of first kind.
  • the vector -ft is constructed from the elements of :
  • the smoothed decode matrix is scaled. In one embodiment, the scaling is performed in the Smooth Decode Matrix block 44, as shown in Fig.4 a). In a different embodiment, the scaling is performed as a separate step in a Scale Matrix block 45, as shown in Fig.4 b).
  • the constant scaling factor is obtained from the decoding matrix.
  • it can be obtained according to the so-called Frobenius norm of the decoding matrix: where d l q is a matrix element in line I and column q of the matrix D (after smoothing).
  • the smoothing and scaling unit 145 as a smoothing unit 1451 for smoothing the first decode matrix D, wherein a smoothed decode matrix D is obtained, and a scaling unit 1452 for scaling smoothed decode matrix D, wherein the decode matrix D is obtained.
  • Fig.6 shows speaker positions in an exemplary 16-speaker setup in a node schematic, where speakers are shown as connected nodes. Foreground connections are shown as solid lines, background connections as dashed lines.
  • Fig.7 shows the same speaker setup with 16 speakers in a foreshortening view.
  • dark areas correspond to lower volumes down to -2dB and light areas to higher volumes up to +2dB.
  • the ratio E/E shows fluctuations larger than 4dB, which is disadvantageous because spatial pans e.g. from top to center speaker position with constant amplitude cannot be perceived with equal loudness.
  • the corresponding panning beam of the center speaker has very small side lobes, which is beneficial for off-center listening positions.
  • the scale (shown on the right-hand side of Fig.12) of the ratio E/E ranges from 3.15 - 3.45dB.
  • fluctuations in the ratio are smaller than 0.31 dB, and the energy distribution in the sound field is very even. Consequently, any spatial pans with constant amplitude are perceived with equal loudness.
  • the panning beam of the center speaker has very small side lobes, as shown in Fig.13. This is beneficial for off center listening positions, where side lobes may be audible and thus would be disturbing.
  • the present invention provides combined advantages achievable with the prior art in [14] and [2], without suffering from their respective disadvantages.
  • each block in the flowchart or block diagrams may represent a module, segment, or portion of code, which comprises one or more executable instructions for implementing the specified logical functions. It should also be noted that, in some alternative implementations, the functions noted in the block may occur out of the order noted in the figures.
  • aspects of the present principles can be embodied as a system, method or computer readable medium. Accordingly, aspects of the present principles can take the form of an entirely hardware embodiment, an entirely software embodiment (including firmware, resident software, micro-code, and so forth), or an embodiment combining software and hardware aspects that can all generally be referred to herein as a "circuit," "module”, or “system.” Furthermore, aspects of the present principles can take the form of a computer readable storage medium. Any combination of one or more computer readable storage medium(s) may be utilized. A computer readable storage medium as used herein is considered a non-transitory storage medium given the inherent capability to store the information therein as well as the inherent capability to provide retrieval of the information therefrom.

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  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Signal Processing (AREA)
  • Multimedia (AREA)
  • Stereophonic System (AREA)
  • Circuit For Audible Band Transducer (AREA)
  • Obtaining Desirable Characteristics In Audible-Bandwidth Transducers (AREA)

Abstract

L'invention concerne la restitution de signaux de champ sonore, telle qu'une ambiophonie d'ordre supérieur (HOA), pour des configurations de haut-parleurs arbitraires, la restitution conduisant à des propriétés de localisation grandement améliorées et préservant l'énergie. Cela est obtenu par un nouveau type de matrice de décodage pour les données de champs sonores, et une nouvelle manière d'obtenir la matrice de décodage. Dans un procédé de restitution d'une représentation de champ sonore audio destiné à des configurations de haut-parleurs spatiaux arbitraires, la matrice de décodage (D) pour la restitution sur un agencement donné de haut-parleurs cibles est obtenue par les étapes d'obtention d'un certain nombre (L) de haut-parleurs cibles, de leurs positions (I), de leurs positions (II) d'un réseau de modélisation sphérique et d'un ordre HOA (N), de génération (141) d'une matrice mixte (G) à partir des positions (II) du réseau de modélisation et des positions (I) des haut-parleurs, de génération (142) d'une matrice de mode (III) à partir des positions (II) du réseau de modélisation sphérique et de l'ordre HOA, de calcul (143) d'une première matrice de décodage (IV) à partir de la matrice mixte (G) et de la matrice de mode (III), et de lissage et de pondération (144, 145) de la première matrice de décodage (IV) avec des coefficients de lissage et de pondération.
PCT/EP2013/065034 2012-07-16 2013-07-16 Procédé et dispositif de restitution d'une représentation de champs sonores audio pour une lecture audio WO2014012945A1 (fr)

Priority Applications (29)

Application Number Priority Date Filing Date Title
EP13737262.9A EP2873253B1 (fr) 2012-07-16 2013-07-16 Procédé et dispositif de restitution d'une représentation de champs sonores audio pour une lecture audio
KR1020237037407A KR20230154111A (ko) 2012-07-16 2013-07-16 오디오 재생을 위한 오디오 음장 표현을 렌더링하는 방법 및 장치
JP2015522078A JP6230602B2 (ja) 2012-07-16 2013-07-16 オーディオ再生のためのオーディオ音場表現をレンダリングするための方法および装置
EP19203226.6A EP3629605B1 (fr) 2012-07-16 2013-07-16 Procédé et dispositif de rendu d'une représentation d'un champ acoustique audio
KR1020207004422A KR102201034B1 (ko) 2012-07-16 2013-07-16 오디오 재생을 위한 오디오 음장 표현을 렌더링하는 방법 및 장치
BR122020017389-0A BR122020017389B1 (pt) 2012-07-16 2013-07-16 Método e dispositivo para renderização de uma representação de campo sonoro de áudio para reprodução de áudio e meio legível por computador
KR1020227044216A KR102597573B1 (ko) 2012-07-16 2013-07-16 오디오 재생을 위한 오디오 음장 표현을 렌더링하는 방법 및 장치
KR1020217000214A KR102479737B1 (ko) 2012-07-16 2013-07-16 오디오 재생을 위한 오디오 음장 표현을 렌더링하는 방법 및 장치
CN201380037816.5A CN104584588B (zh) 2012-07-16 2013-07-16 用于渲染音频声场表示以供音频回放的方法和设备
EP21214639.3A EP4013072B1 (fr) 2012-07-16 2013-07-16 Procédé et dispositif de rendu d'une représentation d'un champ acoustique audio
BR112015001128-4A BR112015001128B1 (pt) 2012-07-16 2013-07-16 Método e dispositivo para renderização de uma representação de um som ou campo sonoro e meio legível por computador
KR1020157000821A KR102079680B1 (ko) 2012-07-16 2013-07-16 오디오 재생을 위한 오디오 음장 표현을 렌더링하는 방법 및 장치
US14/415,561 US9712938B2 (en) 2012-07-16 2013-07-16 Method and device rendering an audio soundfield representation for audio playback
AU2013292057A AU2013292057B2 (en) 2012-07-16 2013-07-16 Method and device for rendering an audio soundfield representation for audio playback
BR122020017399-8A BR122020017399B1 (pt) 2012-07-16 2013-07-16 Método e dispositivo para renderizar uma representação de campo sonoro ambisonics de ordem superior para reprodução de áudio, dispositivo para decodificação e meio legível por computador
EP23202235.0A EP4284026A3 (fr) 2012-07-16 2013-07-16 Procédé et dispositif de rendu d'une représentation d'un champ acoustique audio
HK15111315.8A HK1210562A1 (en) 2012-07-16 2015-11-17 Method and device for rendering an audio soundfield representation for audio playback
AU2017203820A AU2017203820B2 (en) 2012-07-16 2017-06-06 Method and device for rendering an audio soundfield representation for audio playback
US15/619,935 US9961470B2 (en) 2012-07-16 2017-06-12 Method and device for rendering an audio soundfield representation
US15/920,849 US10075799B2 (en) 2012-07-16 2018-03-14 Method and device for rendering an audio soundfield representation
US16/114,937 US10306393B2 (en) 2012-07-16 2018-08-28 Method and device for rendering an audio soundfield representation
AU2019201900A AU2019201900B2 (en) 2012-07-16 2019-03-19 Method and device for rendering an audio soundfield representation for audio playback
US16/417,515 US10595145B2 (en) 2012-07-16 2019-05-20 Method and device for decoding a higher-order ambisonics (HOA) representation of an audio soundfield
US16/789,077 US10939220B2 (en) 2012-07-16 2020-02-12 Method and device for decoding a higher-order ambisonics (HOA) representation of an audio soundfield
US17/189,067 US11451920B2 (en) 2012-07-16 2021-03-01 Method and device for decoding a higher-order ambisonics (HOA) representation of an audio soundfield
AU2021203484A AU2021203484B2 (en) 2012-07-16 2021-05-28 Method and device for rendering an audio soundfield representation for audio playback
US17/943,965 US11743669B2 (en) 2012-07-16 2022-09-13 Method and device for decoding a higher-order ambisonics (HOA) representation of an audio soundfield
AU2023203838A AU2023203838A1 (en) 2012-07-16 2023-06-19 Method and device for rendering an audio soundfield representation for audio playback
US18/359,198 US20240040327A1 (en) 2012-07-16 2023-07-26 Method and device for decoding a higher-order ambisonics (hoa) representation of an audio soundfield

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